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A Practical Guide to 'Free-Energy' Devices

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them, will depend upon the order in which the coils associated with the stationary magnetic members are<br />

energised.<br />

Fig.13 is a circuit diagram for the device shown in Fig.1 and Fig.2, showing the circuit connections for the coils<br />

26-38 and for the circuit elements associated with them. A similar circuit can be used for the construction shown<br />

in Fig.7 and Fig.12. The circuit also includes connections <strong>to</strong> the various pho<strong>to</strong>transis<strong>to</strong>rs and infra red emitters.<br />

In Fig.13, the circuit 120 is shown including a power supply 122 which may be a battery power supply, a rectified<br />

AC power supply or an AC or pulsed power supply. The positive side 124 of the power supply 122 is shown<br />

connected <strong>to</strong> one side of each of the coils 26-38, coil 26 and the circuits associated with it being shown in bold<br />

outline and including connections <strong>to</strong> one side of a resis<strong>to</strong>r 128 and <strong>to</strong> one side of the pho<strong>to</strong> transis<strong>to</strong>rs 58-70. The<br />

opposite side of the coil 26 is connected <strong>to</strong> one terminal of MOSFET 126. The opposite side of the resis<strong>to</strong>r 128 is<br />

connected <strong>to</strong> one side of the infra red emitter 72, as well as <strong>to</strong> the corresponding sides of all of the other infra red<br />

emitters 74-84. The opposite sides of the infra red emitters 72-84 are connected by lead 130 <strong>to</strong> the negative<br />

terminal side 132 of the power supply 122. With the circuit as shown, the infra red emitters 72-84 are all<br />

continuously energised and produce light which can be detected by the respective pho<strong>to</strong>transis<strong>to</strong>rs 58-70 when<br />

one of the openings 48 or 50 passes between them. When this happens, the respective pho<strong>to</strong>transis<strong>to</strong>r 58 will<br />

conduct and in so doing will apply positive voltage on the associated MOSFET 126, turning the MOSFET on, and<br />

causing the voltage of the source 122 <strong>to</strong> also be applied across the coil 26. The circuit for this is from the source<br />

122 through the coil 26, through the MOSFET 126 <strong>to</strong> and through the lead 134 <strong>to</strong> the opposite side of the source<br />

122. When the supply voltage is applied across the coil 26, it operates <strong>to</strong> limit or prevent magnetic<br />

communication between whichever one of the magnets 54 or 56 happens <strong>to</strong> be positioned adjacent <strong>to</strong> the coil 26<br />

which is in the space between that magnet 54 or 56 and the magnet 24. This circuit is shown in bold in Fig.13.<br />

By properly timing and controlling the application of voltage <strong>to</strong> the various coils 26-38 in the manner described,<br />

the magnetic coupling between the magnets 54 and 56 and the magnet 24 can be accurately controlled and<br />

cause angular magnetic attraction between the magnet 54 (or 56) and magnet 24, which angular attraction (or<br />

repulsion) is in a direction <strong>to</strong> cause rotation of the rotating parts of the structure shown in Figs. 1, 2, 7 and 12. It<br />

should be unders<strong>to</strong>od that each of the coils 26-38 will be controlled in the same manner, that is, will have a<br />

voltage appearing across it at the proper time <strong>to</strong> control the direction of the magnetic coupling in a manner <strong>to</strong><br />

produce rotation. The rotating portions will continue <strong>to</strong> rotate and the speed of rotation can be maintained at any<br />

desired speed. Various means can be used <strong>to</strong> control the speed of rotation such as by controlling the timing of<br />

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